Page 183 - Photodetection and Measurement - Maximizing Performance in Optical Systems
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Stability and Tempco Issues

            176   Chapter Eight

                            Cube      Parallel plate  Thick plate    Pellicle





                                Angled
                                        Beams             Absorber    Beams
                                        overlap    Beams displaced    overlap
                                                   laterally
                              Wedge     Wollaston            Grating  Actuated
                                                             +1
                                                      p
                                                      s
                                              Orthogonal     -1
                                              polarizations
                             Beams displaced
                             in angle
                                            Fused fiber


                        Figure 8.13 Selection of beam-splitters used for intensity referencing.




                                                             Amplitudes
                                      Maximum intensity      1              n 1  n 2
                                        2     2
                                     |A |  + |A |  + 2|A ||A |     f
                                                    1
                                             2
                                       1
                                                      2
                           Intensity        4|A | |A |       |A | e  j 1
                                                               1
                                                                   f
                                  2    2       1  2          |A | e  j 2
                               |A |  + |A |                    2
                                      2
                                1
                        Mean
                             Minimum intensity
                                2     2
                              |A |  + |A | – 2|A ||A |
                                              2
                                            1
                                     2
                               1
                                                                              n  - n 2
                                                                               1
                                                                       |A | =
                                                                         1
                                                                              n  + n 2
                                                                               1
                                   Phase Difference D = f  –  f        Amplitude reflection coefficient
                                                    1
                                                       2
                                                                       at normal incidence
                                                                       Air/glass: |A 1 | = 0.2
                        Figure 8.14 Coherent reflection addition in beam-splitters can lead to large intensity split-ratio fluc-
                        tuations, even with small intensity reflection coefficients.
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